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Theoretical study on photophysical properties of a series of functional pyrimidine‐based organic light‐emitting diodes emitters presenting thermally activated delayed fluorescence
Author(s) -
Zhu Qiuling,
Guo Xugeng,
Zhang Jinglai
Publication year - 2019
Publication title -
journal of computational chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.907
H-Index - 188
eISSN - 1096-987X
pISSN - 0192-8651
DOI - 10.1002/jcc.25808
Subject(s) - fluorescence , oled , pyrimidine , photochemistry , diode , series (stratigraphy) , materials science , optoelectronics , chemistry , nanotechnology , optics , physics , stereochemistry , layer (electronics) , paleontology , biology
Issue concerning accurate prediction of the reverse intersystem crossing rate ( k RISC ) is critical for developing novel efficient thermally activated delayed fluorescence (TADF) materials. In this contribution, the k RISC rates from the lowest excited triplet T 1 state to the lowest excited singlet S 1 state were evaluated for five donor‐π‐acceptor‐type pyrimidine‐based TADF emitters using the semiclassical Marcus theory. Both the singlet‐triplet energy difference (Δ E ST ) and spin–orbit coupling ( V ) between the S 1 and T 1 states were investigated by performing the density functional theory (DFT) and time‐dependent density functional theory (TD‐DFT) calculations. In addition, their fluorescence emission wavelengths ( λ em ) were also calculated at the TD‐DFT level. The predicted k RISC and λ em values are found to reproduce well the available experimental findings. The present results reveal that the k RISC rates of molecules possessing the unsymmetrical diphenyl pyrimidine acceptor core are calculated to be slightly larger than those of their analogues with the symmetrical diphenyl pyrimidine. In addition, introducing two tert‐butyl groups into the 2,7‐positions of the donor moiety of the latter is also an effective method for increasing k RISC when designing TADF emitters. Such a difference is related to the nature of the T 1 excited state. A more remarkable charge‐transfer (CT) contribution to the state can achieve a smaller Δ E ST , leading to a more efficient RISC process, and consequently a shorter delayed fluorescence lifetime as observed experimentally. © 2019 Wiley Periodicals, Inc.

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